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Phase Transitions
A Multinational Journal
Volume 79, 2006 - Issue 6-7
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Original Articles

Properties of (Bi1/9Na2/3)(Mn1/3Nb2/3)O3 analysed within dielectric permittivity, conductivity, electric modulus and derivative techniques approach

, , , , &
Pages 447-460 | Received 22 Mar 2006, Accepted 31 Aug 2006, Published online: 28 Nov 2010
 

Abstract

The (Bi1/9Na2/3)(Mn1/3Nb2/3)O3 ceramics with perovskite structure were sintered. The XRD test proved that the samples are cubic (a = 3.920 ± 0.001 Å). Microstructure and atomic composition were determined with a SEM (JSM-5410) equipped with energy dispersion X-ray analyser (ISIS-300). The fluctuation in the chemical composition was found indicating on local disorder. Broadband dielectric spectroscopy in the range 10−1–3 · 107 Hz was applied within the range of 100–650 K. The real, ϵ′(f, T), and imaginary, ϵ″(f, T), parts of complex dielectric permitivity characteristics, both in the temperature and frequency domain, show relaxation processes partially covered by electric conductivity. At high temperatures the electric conductivity exhibits a thermally activated behaviour σ(f, T) ∝ exp(−E a/kT) but the variable range hopping (VRH) dependence σ ∝ exp[−(T 0/T)1/4] is manifested at low temperatures. The derivatives technique in the frequency (∂ log ϵ/∂ log ω) and temperature (∂ log ϵ/∂T) domain enabled various relaxation processes to be distinguished. The data converted to electric modulus representation, M*(f, T) = 1/ϵ*, exhibited clearly resolved relaxation peaks. The relaxation times obtained from the peaks position show a slightly non-Arrhenius temperature behaviour with the activation energy varying in 0.4–0.6 eV range and characteristic time of the electric conductivity relaxation of the order of 10−12 s. The relaxation times can be fitted at better accuracy with the VRH dependence where T 0 are of the order of 108 K. It is shown that the low frequency ac-conductivity converges to dc-conductivity and the relation σ(0) ∼ ωm ∼ τm −1 typical for the disordered solids applies. The conduction current relaxation relationship behaves in accord with the VRH system: σdc ∝ (T/T 0)q (e 2/kT) ωc, where ωc = νph exp[−(T 0/T)1/4] is valid for the locally disordered (Bi1/9Na2/3)(Mn1/3Nb2/3)O3 compound.

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